GR:KvFs & Geodesics: Solving for L & Derivatives

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SUMMARY

The discussion focuses on the derivation and interpretation of geodesics in the context of general relativity, specifically addressing parts c, d, and e of a problem involving the Lagrangian formulation. The equations presented include ##\dot x^c =\frac{ k_c z^2}{R^2}## and the Lagrangian ##L=K -\frac{\dot{z}^2 R^2}{z^2}##, where ##K## is a sum of constants. The participant expresses confusion regarding the explicit formulation of geodesics and the implications of the Lagrangian's sign, indicating a need for clarity on the relationship between the geodesic equations and conserved quantities. The distinction between "write down" and "write down explicitly" is also examined, emphasizing the expectation for explicit solutions in specified coordinates.

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Homework Statement
see below and question attached , parts c to e
Relevant Equations
see below
I am a bit confused with parts c,d,e . In general does ' write down ' the geodesics mean you can leave it in a form ##d/ds( ..) =0## for example here I get 3 equations given by :## \dot x^c =\frac{ k_c z^2}{R^2}## (for## c =t,x,y ##and k is a constant) , and let me use the lagrangian to replace the equation and then I get :## L=K -\frac{\dot{z}^2 R^2}{z^2}## where L will be set## >0 <0 ## or ##=0## depending on whether s-l , t- l etc and K is a sum of the constants ##k_c ^2##

d) the above seems to leave me with a pretty trivial answer to this part which is partly why I'm wondering whether the above is correct or not , since ##L <0 ## and the second term is positive . ( I thought perhaps I may need to look at the ##z## geodesic equation more explicitly and maybe solve for ##z(s) ## or replace it with## \dot{z}## but my ## z ## equation looks non linear and second order ... is the idea to solve for ##z(s) ## here before making a deduction on the conditions for the conserved quantities ?e) again this question makes me question my part c ) since , this again seems pretty trivial :

I'm wondering what the difference between ' write down explicitly ' and ' write down ' . I would interpret explicit as perhaps solving the Euler Lagrange equations and taking the second derivative wrt ##s## etc . But , using this method for all four equations , the value of ##L## is not specified - I.e which type of geodesic . Whereas if I use three Euler Lagrange equations and replace one of them with the lagrangian ( plugging in the other variables that have been solved for etc - Kvfs and constants ) I can specify the nature of the geodesic via the value of ##L## . But then in this case c) and e) are pretty much the same - the only different is specifying the value of L and computing the derivative wrt ##s## for the constant equations via kvfs I would have wrote down for part c) .Many thanks , really appreciated.
 

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I would interpret "write down the geodesic equation for ..." as referring to a differential equation simplified maximally using symmetries and conserved quantities. For the null geodesics, I would think (without doing the exercise) that they expect an explicit formula in the stated coordinates, e.g. that for the exterior Schwarzschild metric in Schwarzschild coordinates, there is a family of spacelike geodesics defined by constant t and angular coordinates, with varying r. I would be expecting that null geodesics simplify to the extent of writing actual equation, rather than diff.eq.
 

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